Hostname: page-component-586b7cd67f-2brh9 Total loading time: 0 Render date: 2024-11-26T18:25:45.478Z Has data issue: false hasContentIssue false

The Cosmic Dust Analyzer: Experimental Evaluation of an Impact Ionization Model

Published online by Cambridge University Press:  12 April 2016

J. F. Friichtenicht
Affiliation:
TRW SystemsRedondo Beach, California
N. L. Roy
Affiliation:
TRW SystemsRedondo Beach, California
D. G. Becker
Affiliation:
TRW SystemsRedondo Beach, California

Abstract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

Determination of the elemental composition of cosmic dust particles by means of an impact ionization time-of-flight mass spectrometer has been investigated at several institutions. In most configurations, the instrument supplies the identity of ion groups of both target and particle materials extracted from the impact plasma and the number of ions contained in each group. Experiments have shown that the fractional ionization of a given species is not constant with impact velocity nor is the fractional ionization the same for different kinds of atoms. A model of the impact ionization effect developed at TRW involves an equilibrium plasma condition with the consequence that the fractional ionization for an arbitrary atomic species can be specified by the Saha equation if the plasma volume (V) and temperature (T) are known. It follows that T can be determined by taking the ratio of the Saha equations for two elements present in the target in known concentration. (Taking the ratio negates the requirement of knowing V.) Given T, the procedure can be reversed to yield the relative abundance of elements contained in the impacting particle. To test the model, a PbZrO3-PbTiO3 target was bombarded with high velocity Fe, MoB, and NiAl particles and the number of Pb, Ti, and Zr ions was determined in a time-of-flight mass spectrometer. For each event, the relative abundance of Ti to Pb was taken as known (from electron microprobe analysis) and T was determined from the Ti-Pb measurement. The Zr to Pb ratio was found to be in good agreement with the microprobe analysis (0.38 calculated mean value compared to 0.34 actual). The result was valid for all particle materials and for a velocity range 17<v<47 km/s. T ranged from 3300 to 11 500° K and was only mildly velocity dependent.

Type
Research Article
Copyright
Copyright © NASA 1971

References

Aller, L. H., 1963. Astrophysics—The Atmosphere of the Sun and Stars, second edition, The Ronald Press Co., New York, 115117.Google Scholar
Auek, S., and Sitte, K., 1968. Detection technique for micrometeoroids using impact ionization, Earth Planet. Sci. Letters, 4, 178183.Google Scholar
Friichtenicht, J. F., 1962. Two-million-volt electrostatic accelerator for hypervelocity research, Rev. Sci. Instr., 33, 209212.Google Scholar
Friichtenicht, J. F., and Slattery, J. C., 1963. Ionization associated with hypervelocity impact, NASA Tech. Note D-2091.Google Scholar
Hansen, D. O., 1968. Mass analysis of ions produced by hypervelocity impact, Appl. Phys. Letters, 13, 8991.Google Scholar
Hansen, D. O., and Roy, N. L., 1966. A solid-state low-noise preamplifier, Nucl. Instr. Methods, 40, 209212.Google Scholar
Roy, N. L., and Becker, D. G., 1971. A time interval selector and proportional delay generator, Rev. Sci. Instr., 42, 204209.CrossRefGoogle Scholar
Shelton, H., Hendricks, C. D. JR., and Wuerker, R. F., 1960. Electrostatic acceleration of microparticles to hypervelocities, J. Appl. Phys., 31, 12431246.Google Scholar
Sutton, G. W., and Sherman, A., 1965. Engineering Magnetohydrodynamics, McGraw-Hill Book Co., New York, 225.Google Scholar